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The input transfer coefficients describe how applied fields (input fields) \
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This tutorial details the three methods to compute the input transfer \
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Load the interfacial thin film nonlinear spectroscopy package\
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Implementation of the input transfer coefficients in the \
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Cell["\<\
Of primary interest is that the three methods to compute the local fields at \
any interface within a thin film system will all give the same result.  We \
start by showing this is indeed the case but without going into details of \
how each method is computed.  Taking the model system of an organic \
semiconductor thin film deposited on a dielectric thin film and semiconductor \
substrate, we can compute the input transfer coefficient for an 800 nm input \
beam incident from the top side of the system.  In the next section we will \
detail how each method works.\
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Fig.2 Illustration of the model 2-layer system with input beam incident from \
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Numerically compute input transfer coeffients at all three interfaces for an \
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coefficients, and by treating the polarized sheet as a finite layer in the \
stack and take the limit of 0 thickness.\
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We have numerically verified that all three methods give identical local \
fields at all three interfaces.  The next section details how each method \
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Of the three methods to compute the input transfer coefficients, two of these \
arrive at the local fields by calculating adjacent fields and applying \
boundary conditions, while the third relies on treating the interfacial \
polarized sheet as a finite layer in the thin film stack.  We begin by \
detailing methods that use adjacent fields.\
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The first two methods to compute the input transfer coefficients rely on \
calculating the field amplitudes for the waves moving towards and away from a \
point on an interface and then use standard boundary conditions from \
electromagnetic theory to determine the local field at the interface.  \
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